全文获取类型
收费全文 | 6513篇 |
免费 | 1128篇 |
国内免费 | 1608篇 |
专业分类
测绘学 | 964篇 |
大气科学 | 1573篇 |
地球物理 | 1484篇 |
地质学 | 2886篇 |
海洋学 | 990篇 |
天文学 | 57篇 |
综合类 | 450篇 |
自然地理 | 845篇 |
出版年
2024年 | 46篇 |
2023年 | 114篇 |
2022年 | 230篇 |
2021年 | 275篇 |
2020年 | 282篇 |
2019年 | 320篇 |
2018年 | 240篇 |
2017年 | 313篇 |
2016年 | 334篇 |
2015年 | 313篇 |
2014年 | 395篇 |
2013年 | 425篇 |
2012年 | 387篇 |
2011年 | 391篇 |
2010年 | 351篇 |
2009年 | 411篇 |
2008年 | 419篇 |
2007年 | 502篇 |
2006年 | 408篇 |
2005年 | 396篇 |
2004年 | 360篇 |
2003年 | 284篇 |
2002年 | 267篇 |
2001年 | 235篇 |
2000年 | 237篇 |
1999年 | 200篇 |
1998年 | 181篇 |
1997年 | 166篇 |
1996年 | 155篇 |
1995年 | 107篇 |
1994年 | 116篇 |
1993年 | 89篇 |
1992年 | 78篇 |
1991年 | 57篇 |
1990年 | 41篇 |
1989年 | 31篇 |
1988年 | 28篇 |
1987年 | 16篇 |
1986年 | 12篇 |
1985年 | 7篇 |
1984年 | 2篇 |
1983年 | 3篇 |
1982年 | 3篇 |
1981年 | 2篇 |
1980年 | 9篇 |
1979年 | 3篇 |
1978年 | 4篇 |
1977年 | 1篇 |
1971年 | 1篇 |
1954年 | 2篇 |
排序方式: 共有9249条查询结果,搜索用时 0 毫秒
81.
铜山—石砀山铜钼矿位于江苏宁镇山脉中段龙潭—仓头背斜南翼,矿体主体受接触带构造控制。以往地质工作缺少深部研究,对物化探异常再解释工作不够,物探方法找矿专属性研究不细致,综合研究程度较浅。综合分析铜山—石砀山地区地质、物性资料,采用1∶2 000高精度磁法测量、可控源音频大地电磁测深剖面等物探技术,圈定地磁异常8个(C1—C8),推断由2个磁性地质体、8个矽卡岩体引起。择优对C2异常进行了钻探验证。研究认为该区可控源音频大地电磁测深高低阻过渡带部位的磁异常具有重要的找矿意义,即该区中酸性岩体与碳酸盐岩接触带部位具有含铜钼磁铁矿形成的有利地质条件。对比分析研究区及周边找矿信息,认为铜山—石砀山地区找矿深部有潜力,外围有远景。 相似文献
82.
83.
模拟地震波传播的三维逐元并行谱元法 总被引:2,自引:0,他引:2
高效地震波场正演模拟对于复杂模型中地震波传播与成像研究至关重要.本文在谱元法原理框架内,对已有逐元谱元法改进,提出一种新的逐元并行谱元法求解三维地震波运动方程,并得到地震波场.逐元并行谱元法的核心思想在于在单元上进行质量矩阵与解向量的乘积运算,并将此运算平均分配至每一个CPU计算核心,此处理有利提升谱元法的并行计算效率.同时,根据Gauss-Lobatto-Legendre (GLL)数值积分点与插值点重合的特点,将稠密单元刚度矩阵的存储转化成单元雅克比矩阵行列式的值及其逆的存储,大幅减少谱元法计算内存开销.此外,在模型边界上利用逐元并行谱元法求解二阶位移形式完美匹配层(PML)吸收边界条件,消除边界截断而引入的虚假反射.通过逐元并行谱元法得到的数值解与解析解对比,以及实际地震波场模拟,数值结果证实了逐元并行谱元法用于地震波场模拟的高效性.
相似文献84.
85.
Application of Dynamic Subgrid-scale Models for Large-eddy Simulation of the Daytime Convective Boundary Layer over Heterogeneous Surfaces 总被引:1,自引:0,他引:1
The sensitivity of large-eddy simulation (LES) to the representation of subgrid-scale (SGS) processes is explored for the
case of the convective boundary layer (CBL) developing over surfaces with varying degrees of spatial heterogeneity. Three
representations of SGS processes are explored: the traditional constant Smagorinsky–Lilly model and two other dynamic models
with Lagrangian averaging approaches to calculate the Smagorinsky coefficient (C
S
) and SGS Prandtl number (Pr). With initial data based roughly on the observed meteorology, simulations of daytime CBL growth are performed over surfaces
with characteristics (i.e. fluxes and roughness) ranging from homogeneous, to striped heterogeneity, to a realistic representation
of heterogeneity as derived from a recent field study. In both idealized tests and the realistic case, SGS sensitivities are
mostly manifest near the surface and entrainment zone. However, unlike simulations over complex domains or under neutral or
stable conditions, these differences for the CBL simulation, where large eddies dominate, are not significant enough to distinguish
the performance of the different SGS models, irrespective of surface heterogeneity. 相似文献
86.
87.
研究了用GPS测定基阵坐标,分析了水听器基阵所接收到的声脉冲信号的处理。通过模拟和实测数据的试算,证明了本文提出的模型及方法不但能处理多系统含有粗差的观测值,而且具有良好的跟踪处理机动目标的性能。 相似文献
88.
Paleo‐fires and Atmospheric Oxygen Levels in the Latest Permian: Evidence from Maceral Compositions of Coals in Eastern Yunnan,Southern China 总被引:1,自引:0,他引:1
Inertinite maceral compositions of the Late Permian coals from three sections in the terrestrial and paralic settings of eastern Yunnan are analyzed in order to reveal the paleo-fire events and the atmospheric oxygen levels in the latest Permian. Although the macerals in the studied sections are generally dominated by vitrinite, the inertinite group makes up a considerable proportion. Its content increases upward from the beginning of the Late Permian to the coal seam near the Permian-Triassic boundary. Based on the microscopic features and the prevailing theory that inertinite is largely a by-product of paleo-fires, we suggest that the increasing upward trend of the inertinite abundance in the latest Permian could imply that the Late Permian peatland had suffered from frequent wildfires. Since ignition and burning depend on sufficient oxygen, a model-based calculation suggests that the O2 levels near the Wuchiapingian/Changhsingian boundary and the Permian-Triassic boundary are 27% and 28% respectively. This output adds supports to other discoveries made in the temporal marine and terrestrial sediments, and challenges the theories advocating hypoxia as a mechanism for the Permian-Triassic boundary crisis. 相似文献
89.
Previous work has shown that ionospheric HF radar backscatter in the noon sector can be used to locate the footprint of the magnetospheric cusp particle precipitation. This has enabled the radar data to be used as a proxy for the location of the polar cap boundary, and hence measure the flow of plasma across it to derive the reconnection electric field in the ionosphere. This work used only single radar data sets with a field of view limited to 2 h of local time. In this case study using four of the SuperDARN radars, we examine the boundary determined over 6 h of magnetic local time around the noon sector and its relationship to the convection pattern. The variation with longitude of the latitude of the radar scatter with cusp characteristics shows a bay-like feature. It is shown that this feature is shaped by the variation with longitude of the poleward flow component of the ionospheric plasma and may be understood in terms of cusp ion time-of-flight effects. Using this interpretation, we derive the time-of-flight of the cusp ions and find that it is consistent with approximately 1 keV ions injected from a subsolar reconnection site. A method for deriving a more accurate estimate of the location of the open-closed field line boundary from HF radar data is described. 相似文献
90.
A monoclinic KAlSi3O8 feldspar Manebach twin boundary was synthesized by diffusion bonding and examined using high-resolution transmission electron
microscopy. The sharp (001) twin boundary is straight and free of strain. The boundary width is smaller than d001. There is no rigid body shift observed at the twin boundary, and the feldspar structure is arranged symmetrically across
(001). The twin boundary structure consists of bridged tetrahedral crankshafts, which are characteristic of the feldspar lattice.
The grain boundary structure is in good agreement with the geometrical model of Taylor et al. (1934). The grain boundary composition
of K1/2H1/2AlSi3O8 differs from their model.
Received: 13 February 2002 / Accepted: 24 December 2002
Acknowledgements We thank M. Rühle, S. Hutt, J. Mayer, A. Strecker and U. Salzberger at MPI, Stuttgart, for their support and valuable advice
in preparing TEM sections of bicrystals. 相似文献